Consider the following equivalent form of the sequence (
8).
$$\begin{aligned} \xi _0=0, \; \xi _{k+1}=\xi _k-\varLambda _h^{-1}(F(x_0+h+\xi _k)),\quad k=0,1,2,\dots . \end{aligned}$$
We prove that
\(\forall _k \Vert \xi _{k+1}-\xi _k\Vert \le \frac{1}{2}\Vert \xi _k-\xi _{k-1}\Vert \). For this purpose we define a multivalued mapping
\(\varPhi _{h}: U_{\varepsilon }(x_{0})\rightarrow 2^{\mathbb {R}^n},\) such that
$$\begin{aligned}&\varPhi _{h}(x)\in x -\varLambda ^{-1}_h(f_{1}(x_{0}+h+x)+\cdots + f_{p}(x_{0}+h+x))\\&\quad =x -\varLambda ^{-1}_h(F(x_{0}+h+x)), \quad x\in U_{\varepsilon }(x_{0}). \end{aligned}$$
The sets
\(\varPhi _{h}(x)\) are non-empty because
\(\varLambda _h\) is a surjection for any
\(x\in U_{\varepsilon }(x_{0}).\) Moreover, for any
\(y\in Y_{1}\times \cdots \times Y_{p}\) the sets
\(\varLambda ^{-1}_h(y)\) are linear manifolds parallel to
\(\mathrm{Ker}\varLambda _h,\) and hence the sets
\(\varPhi _{h}(x)\) are closed for any
\(x\in U_{\varepsilon }(x_{0}).\) Taking into account Remark
2 we can write
\(\Vert \xi _{k+1}-\xi _k\Vert =\mathrm{dist}\left( \varPhi _{h}(\xi _{k+1}),\varPhi _{h}(\xi _{k})\right) \). We prove that
$$\begin{aligned} \mathrm{dist}\left( \varPhi _{h}(\xi _{k+1}),\varPhi _{h}(\xi _{k})\right) \le \frac{1}{2} \Vert \xi _{k}-\xi _{k-1}\Vert , \end{aligned}$$
(10)
for
\(\xi _{k+1},\xi _{k}\in U_{\frac{\varepsilon }{2}}(x_{0})\) such that
\(\Vert \xi _{j}\Vert \le \frac{\Vert h\Vert }{R},\)
\(j=k,k+1,\) where
$$\begin{aligned} R=\max \limits _i R_{i}, R_{i}= \max \left\{ 1,\frac{2}{\varepsilon \cdot c_{2}}\cdot \frac{1}{(i-1)!}\left\| f^{(i)}_{i}(x_{0})\right\| \right\} ,\quad i=1,\ldots ,p. \end{aligned}$$
Let
\(\varLambda _{h,i}=\frac{1}{(i-1)!}f_{i}^{(i)}(x_{0})[h]^{i-1}, \; i=1,\ldots ,p\),
\(s_{1}=x_{0}+h+\xi _{k},\)
\(s_{2}=x_{0}+h+\xi _{k-1}.\) Then
$$\begin{aligned}&\mathrm{dist}\left( \varPhi _{h}(\xi _{k+1}),\varPhi _{h}(\xi _{k})\right) = \inf \left\{ \Vert z_{1}-z_{2}\Vert :z_{1}\in \varPhi _{h}(\xi _{k}),\;z_{2}\in \varPhi _{h}(\xi _{k+1})\right\} \\&\quad =\inf \left\{ \Vert z_{1}-z_{2}\Vert :\varLambda _h(z_{i+1})=\varLambda _h(\xi _{k-i})- \left( f_{1}(s_{i+1})+\cdots +f_{p}(s_{i+1})\right) ,\;i=0,1\right\} \\&\quad \le \inf \left\{ \Vert z\Vert :\varLambda _h(z)=\varLambda _h(\xi _{k}-\xi _{k-1})- \left( f_{1}(s_{1})-f_{1}(s_{2})+\cdots +f_{p}(s_{1})- f_{p}(s_{2})\right) \right\} \\&\quad =\inf \Bigg \{\Vert z\Vert :\varLambda _h(z)= \Bigg (\varLambda _{h,1}(\xi _{k}-\xi _{k-1})-f_{1}(s_{1})+f_{1}(s_{2})\\&\qquad +\cdots +\frac{1}{\Vert h\Vert ^{p-1}}\left( \varLambda _{h,p}(\xi _{k}-\xi _{k-1})-f_{p}(s_{1})+ f_{p}(s_{2})\right) \Bigg )\Bigg \}\\&\quad \le \inf \Bigg \{\Vert z\Vert :z= \varLambda ^{-1}_h\Bigg (\varLambda _{h,1}(\xi _{k}-\xi _{k-1})-f_{1}(s_{1})+f_{1}(s_{2})\\&\qquad +\cdots +\frac{1}{\Vert h\Vert ^{p-1}}\left( \varLambda _{h,p}(\xi _{k}-\xi _{k-1})-f_{p}(s_{1})+ f_{p}(s_{2})\right) \Bigg )\Bigg \}\\&\quad \le c_{1}\cdot \sum _{i=1}^{p}\frac{1}{\Vert h\Vert ^{i-1}}\left\| f_{i}(s_{1})-f_{i}(s_{2})- \varLambda _{h,i}(s_{1}-s_{2})\right\| . \end{aligned}$$
Taking into account Lemma
3, we have
$$\begin{aligned}&\left\| f_{i}(s_{1})-f_{i}(s_{2})-\varLambda _{h,i}(s_{1}-s_{2})\right\| \nonumber \\&\quad \le \sup _{\theta \in [0,1]}\left\| f_{i}'(s_{2} +\theta (s_{1}-s_{2}))-\varLambda _{h,i}\right\| \cdot \left\| \xi _{k}-\xi _{k-1}\right\| .\;\;\;\;\;\;\;\;\;\;\; \end{aligned}$$
(11)
As
\(f_{i}\) is completely degenerate up to the order
i we obtain the following Taylor expansion
$$\begin{aligned}&f_{i}'(s_{2}+\theta (s_{1}-s_{2}))\\&\quad =f_{i}'(x_{0})+\ldots +\frac{f_{i}^{(i)} (x_{0})[s_{2}-x_{0}+\theta (s_{1}-s_{2})]^{i-1}}{(i-1)!}+\omega _{i}(h,\xi _{k},\xi _{k-1},\theta )\nonumber \\&\quad = \frac{f_{i}^{(i)} (x_{0})[s_{2}-x_{0}+\theta (s_{1}-s_{2})]^{i-1}}{(i-1)!}+\omega _{i}(h,\xi _{k},\xi _{k-1},\theta ),\nonumber \end{aligned}$$
(12)
where
$$\begin{aligned} \left\| \omega _{i}(h,\xi _{k},\xi _{k-1},\theta )\right\| \le \sup _{x\in U_{\varepsilon }(x_{0})} \left\| f_{i}^{(i+1)}(x)[h+\xi _{k-1}+\theta (s_{1}-s_{2})]^{i}\right\| . \end{aligned}$$
Moreover,
$$\begin{aligned}&f_{i}^{(i)} (x_{0})[s_{2}-x_{0}+\theta (s_{1}-s_{2})]^{i-1}=f^{(i)}_{i}(x_{0})[h+\xi _{k-1}+\theta (s_{1}-s_{2})]^{i-1} \nonumber \\&\quad =\sum _{t=0}^{i-1}\left( ^{i-1} _{\;\;t}\right) f^{(i)}_{i}(x_{0})[h]^{i-1-t}[\xi _{k-1}+\theta (s_{1}-s_{2})]^{t}\\&\quad =f^{(i)}_{i}(x_{0})[h]^{i-1}+\sum _{t=1}^{i-1}\left( ^{i-1} _{\;\;t}\right) f^{(i)}_{i}(x_{0})[h]^{i-1-t} [\xi _{k-1}+\theta (s_{1}-s_{2})]^{t}. \nonumber \end{aligned}$$
(13)
Thus, inserting (
14) into (
13) and then putting the obtained formula into (
11), we get
$$\begin{aligned}&\left\| f_{i}(s_{1})- f_{i}(s_{2})-\varLambda _{h,i}(s_{1}-s_{2})\right\| \nonumber \\&\quad \le \sup _{\theta \in [0,1]}\left\| \frac{\sum _{t=1}^{i-1}\left( ^{i-1} _{\;\;t}\right) f^{(i)}_{i}(x_{0})[h]^{i-1-t} [\xi _{k}+\theta (s_{1}-s_{2})]^{t}}{(i-1)!}+\omega _i(h,\xi _{k},\xi _{k-1},\theta )\right\| \nonumber \\&\qquad \cdot \left\| \xi _{k}-\xi _{k-1}\right\| . \end{aligned}$$
(14)
Let
\(F(x_{0})=(y_{1},\ldots ,y_{p}),\) where
\(y_{i}\in Y_{i}, \; i=1, \ldots ,p.\) Then from the assumption and the definition of norm in
\(\mathbb {R}^n\) we have
\(\Vert y_{1}\Vert +\cdots +\Vert y_{p}\Vert \le \delta .\) As
\(R\Vert \xi _{j}\Vert \le \Vert h\Vert ,\)
\(j=k-1,k\) we have
\(\left\| h+\xi _{k-1}+\theta (s_{1}-s_{2})\right\| \le 4 \Vert h\Vert .\) Taking into account Lemma
4 and assumptions (3) and (2) of Theorem
2 we have
$$\begin{aligned} \Vert h\Vert\le & {} (1+\varDelta ) \Vert \varPsi ^{-1}(-F(x_{0}))\Vert \le (1+\varDelta )c_{3} p \left( \Vert y_{1}\Vert +\cdots +\Vert y_{p}\Vert ^{\frac{1}{p}}\right) \\\le & {} (1+\varDelta )c_{3} p^{2}\delta ^{\frac{1}{p}}\le \frac{\varepsilon }{2}, \end{aligned}$$
where
\(0<\varDelta <\frac{1}{2}.\) This and the previous formulae imply
$$\begin{aligned} \left\| \omega _{i}(h,\xi _{k},\xi _{k-1},\theta )\right\| \le c_{2} \Vert h+\xi _{k-1}+\theta (s_{1}-s_{2})\Vert ^{i}\le 4^{i} c_{2} \frac{\varepsilon }{2}\Vert h\Vert ^{i-1}. \end{aligned}$$
(15)
Moreover,
$$\begin{aligned} \Vert \xi _{k-1}+\theta (s_{1}-s_{2})\Vert \le 3 \Vert h\Vert /R\le 3 \Vert h\Vert /R_{i}. \end{aligned}$$
(16)
Taking into account the definition of
\(R_{i}\), we get
$$\begin{aligned}&\left\| \sum _{k=1}^{i-1}\left( ^{i-1} _{\;\;k}\right) f^{(i)}_{i}(x_{0})[h]^{i-1-k}[\xi _{k-1}+\theta (s_{1}-s_{2})]^{k}\right\| \nonumber \\&\quad \le \left\| f^{(i)}_{i}(x_{0})\right\| \cdot \sum _{k=1}^{i-1}\left( ^{i-1} _{\;\;k}\right) \Vert h\Vert ^{i-1-k}(3 \Vert h\Vert )^{k}/R^{k}_{i}\nonumber \\&\quad \le \left\| f^{(i)}_{i}(x_{0})\right\| \cdot \Vert h\Vert ^{i-1}\cdot 4^{i-1}/R_{i}\le 4^{i}(i-1)! \frac{\varepsilon }{2} c_{2} \Vert h\Vert ^{i-1}. \end{aligned}$$
(17)
Now, inserting (
15)–(
17) into (
14) we obtain
$$\begin{aligned} \left\| f_{i}(s_{1})-f_{i}(s_{2})-\varLambda _{h,i} (s_{1}-s_{2})\right\| \le 4^{i}\varepsilon c_{2}\Vert h\Vert ^{i-1}\cdot \Vert \xi _{k}-\xi _{k-1}\Vert . \end{aligned}$$
Hence
$$\begin{aligned}&\Vert \xi _{k+1}-\xi _{k}\Vert \le c_{1} \cdot \sum _{i=1}^{p}\frac{1}{\Vert h\Vert ^{i-1}}4^{i} c_{2} \varepsilon \Vert h\Vert ^{i-1} \Vert \xi _{k}-\xi _{k-1}\Vert \\&\quad =\frac{4}{3}\left( 4^{p}-1\right) c_{1} c_{2}\varepsilon \Vert \xi _{k}-\xi _{k-1}\Vert \le \frac{1}{2} \Vert \xi _{k}-\xi _{k-1}\Vert \end{aligned}$$
which proves (
10).